TRAINING COURSE ON RADIATION DOSIMETRY:

Instrumentation 1 –

Gas detectors / Part 1Anthony WAKER,

University of Ontario Instutute of TechnologyWed. 21/11/2012, 15:00 – 16:00 pm, and 16:30 – 17:30 pm

• One of the oldest and most widely used radiation detectors

• Gas-filled detectors sense the direct ionization created by the passage of charged particles caused by the interaction of the radiation with the chamber gas

Ion Chambers Proportional Counters Geiger-Mueller Counters

GAS-FILLED DETECTORS

BASIC COMPONENTS OF AN IONIZATION CHAMBER

Common Fill Gases: Ar, He, H2, N2, Air, O2, CH4, TE

To create an ion pair, a minimum energy equal to the ionization energy of the gas molecule must be transferred

Ionization energy between 10 to 25 eV for least tightly bound electron shells for gases of interest

Competing mechanisms such as excitation leads to incident particle energy loss without the creation of ion pair

W-value: average energy lost by incident particle per ion pair formed

IONIZATION IN GASES

Typical W-values are in the range of 25 – 35 eV/ion pair

Under steady-state irradiation, rate of ion-pair formation is constant

For a small test volume, rate of formation will be exactly balanced by rate at which ion pairs are lost from volume due to recombination, diffusion or migration from the volume.

CHARGE COLLECTION

For ions in a gas,

CHARGE COLLECTION

+ve and –ve charges are swept towards their respective electrodes with

By increasing concentration of ions within the gas volume decreases suppressing volume recombination within the gas volume.

Two types of recombination:

Columnar (or initial) recombinationIncreases with LET of Radiation

Volume recombinationIncreases with dose-rate

RECOMBINATION

𝑑𝑛+¿

𝑑𝑡+𝑑𝑛

−

𝑑𝑡=−𝛼𝑛+¿𝑛−¿¿

CHARGE COLLECTION

IONIZATION CHAMBER – FARMER CHAMBER

IONIZATION CHAMBERS

What ionization current would we expect to measure in a Farmer chamber placed in a high energy photon radiotherapy beam where the dose rate to air is 10 Gy per minute.

Typical ionization currents are extremely small.Require good insulation and guard rings to ensure leakage current does not interfere with ionization current

INSULATORS AND GUARD RINGS

IONIZATION CHAMBER DOSIMETRY

DOSIMETRY WITH IONIZATION CHAMBERS

𝐷𝑚𝑎𝑡𝑡𝑒𝑟=𝐷𝑐𝑎𝑣𝑖𝑡𝑦 . {𝑆𝜌 }𝑚𝑎𝑡𝑡𝑒𝑟𝑐𝑎𝑣𝑖𝑡𝑦

FANO’S THEOREM

In an infinite medium of given atomic composition exposed to a uniform field of indirectly ionizing radiation, the field of secondary radiation is also uniform and independent of density of the medium, as well as density variations from point to point.

This means that if an ionization chamber is constructed of a wall material and filled with gas of the same atomic composition the dose to the wall material will be the same as the dose measured to the gas regardless of the size of the chamber

IONIZATION CHAMBER DOSIMETRY - CALIBRATION

IONIZATION CHAMBER DOSIMETRY

TISSUE E

QUIVALENT P

ROPORTIONAL C

OUNTERS

TEPC

DOSIMETRY W

ITH G

AS

IONIZ

ATION D

EVISES

ATOMIC COMPOSITION OF TISSUE AND TE GAS

ICRU Tissue (Muscle) atomic composition by % weight

H C N O

10.2 12.3 3.5 72.9

• Methane based• CH4 (64.4% partial pressure)

• CO2 (32.4% partial pressure)

• N2 (3.2% partial pressure)

• By %weight: H (10.2); C (45.6); N (3.5); O (40.7)

• Propane based• C3H8 (% partial pressure)

• CO2 (% partial pressure)

• N2 (%partial pressure)

• By %weight: H (10.3); C (56.9); N (3.5); O (29.3)

TISSUE EQUIVALENT PLASTIC

A150 TE-plastic atomic composition by % weight

The main tissue equivalent plastic used in dosimetry is A150.

The atomic composition of A150 is close to tissue but has a higher percentage by weight of carbon, which makes it conductive.

H C N O

muscle(10.2)

muscle(12.3)

muscle(3.5)

muscle(72.9)

10.1 77.6 3.5 5.2

GAS-GAIN IN PROPORTIONAL COUNTERS

A proportional counter is a gas-ionization device consisting of a cathode, thin anode wire and fill-gas. Ionization in the fill gas is multiplied providing an amplified signal proportional to the original amount of ionization.

GAS GAIN

The gas-gain achievable in a proportional counter is determined by the first Townsend coefficient α for the counter fill gas used

α itself depends on the reduced electric field in the counter, which is determined by the applied voltage and counter geometry

dG )ln(

GAS GAIN

To a first approximation the relationship between the logarithm of gas-gain and applied anode voltage is linear

0 100 200 300 400 500 600 700 8000

1

2

3

4

5

6

7

8

Relative Gas Gain for Propane Based TE Gas at Pressures 3.25 (graph 1), 6.5 (2), 16.25 (3), 26 (4), 32.5 torr, Relative to the Mea-

surement Made at 32.5 Torr and Vanode 100 V

Series1

Series3

Series5

Series7

Series9

V anode (V)

ln G

*

SIMULATION USING A GAS CAVITY

SITE-SIZE SIMULATION

Energy deposited in the gas cavity by a charged particle crossing the cavity equals energy deposited in tissue site by an identical particle

EtEg

SITE-SIZE SIMULATION

( 1𝜌.𝑑𝐸𝑑𝑥 ) .𝜌 𝑔 .∆𝑔=( 1

𝜌.𝑑𝐸𝑑𝑥 ) .𝜌 𝑡 .∆ 𝑡

tissuegas

𝐸𝑔=𝐸𝑡

SITE-SIZE SIMULATION

The density of the gas in the cavity is adjusted to equal the ratio of the tissue site diameter to the gas cavity diameter

tg

tg X

X

Density of Gas

Diameter of Gas Cavity

Density of Tissue Site (1000 kg.m-3)

Diameter of Tissue Site

EXAMPLE

What is the density of propane TE gas required for a 1 cm cavity to simulate a tissue sphere of 1 µm.

= 10-4 . 1000 kg.m-3 = 0.1kg.m-3

EXAMPLE

What pressure of propane TE gas is required for a density of 0.1 kg.m-3

At 20 oC:

(41.72 torr)

Rossi Counter

TEPC CALIB

RATION

I NT

ER

NA

L AL P

HA

SO

UR

CE

S

INTERNAL SOURCE CALIBRATION

In crossing the TEPC an alpha particle will lose an average amount of energy that can be calculated using range-energy data

INTERNAL SOURCE CALIBRATION

Each alpha particle crossing the counter generates a pulse height proportional to the energy deposited; the mean of this distribution is associated with the mean energy deposited in the counter

EXAMPLE

Applied Voltage 750V; amplifier gain 10

Mean energy lost 168.48 keV

Mean chord-length 1.33 µm

Channel 3835 corresponds to 126.68 keV/µm

Calibration Factor for amplifier setting of 10 (126.68/3835) = 0.03303 keV/µm/channel

Using range-energy data for propane based TE gas for a 2 micron simulated diameter and a Cm-244 internal alpha source of energy 5.8 MeV.

Frequency distribution measured in an Am-Be field with a 2” REM500 TEPC with simulated diameter 2µm and calibration factor 1.641keV/µm/chn

Frequency x lineal energy: Dose Distribution d(y) with calibration factor 1.641keV/µm/chn

y.f(y) data plotted in equal logarithmic intervals, 50 per decade

TEPC MEASURABLE

QUANTITIE

S

MEASUREABLE QUANTITIES – AMBIENT DOSE EQUIVALENT

𝐻∗(10)=𝐷∗(10).𝑄Estimated directly from the measured event-size spectrum

Determined from the shape of the event-size spectrum and assuming Q(y) = Q(L)

TEPC MEASUREABLE QUANTITIES – ABSORBED DOSE

From ICRP 60

Assuming that Lineal Energy y is equal to Linear Energy Transfer L

TEPC RESPONSE – KERMA

TEPC ENERGY RESPONSE – QUALITY FACTOR

DETECTORS OTHER T

HAN

TEPCs

GA

S E

L EC

TR

ON

MU

L TI P

L I ER

S

GEMS

GAS ELECTRON MULTIPLIER

Operates as proportional counter except multiplication takes place between the top and bottom surfaces of the GEM structure through microscopically etched holes

Dubeau and Waker Radiat. Prot. Dosim. 128(4), 2008

Dubeau and Waker Radiat. Prot. Dosim. 128(4), 2008

GEM SUMMARY

GEMs can be configured to operate as TEPC and have the advantage of smaller physical size for each detecting element and smaller

simulated diameters for improving dose equivalent response (better LET spectrometers)

Potential for basis as a personal neutron dosimeter

Particle tracking capability depending on read-out pattern of anode

Much work still to be done!